Synthesis of Porous Si/SiO2/C Particles as Anode Materials of Lithium-Ion Batteries

Citation: Deren Yang (2014) Synthesis of Porous Si/Sio2/C Particles as Anode Materials of Lithium-Ion Batteries. J Nanotech Smart Mater 1: 1-4 *Corresponding author: Deren Yang, State Key Lab of Silicon Materials and Department of Materials Science and Engineering, Cyrus Tang Center for Sensor Materials and Applications, Zhejiang University, Hangzhou 310027, People’s Republic of China, E-mail: mseyang@zju.edu.cn


Introduction Abstract
We demonstrate the synthesis of the porous Si/SiO 2 /C particles by the oxidation of Mg 2 Si and subsequent deposition of carbon layers. When used as anode materials of lithium-ion batteries, the porous Si/SiO 2 /C particles deliver a capacity of 550 mAhg -1 after 30 cycles at a current of 800 mAg-1, which is better than bulk Si particles. The enhanced electrochemical performance is ascribing to the porous and core-shell structures. Moreover, the silicon dioxides layer is beneficial to the stability of the SEI film, and the carbon layer and the porous structures can buffer the volume change during the charge/discharge process, which may be responsible the enhanced performance.

Journal of Nanotechnology and Smart Materials
J Nanotech Smart Mater 2014 | Vol 1: 202 Silicon (Si) is one of the most promising anode materials for next-generation lithium-ion (Li-ion) batteries, which has the highest specific capacity of ~4200 mAhg -1 [1]. However, there are two main drawbacks of Si anode materials: the first one is the large volume expansion up to nearly 400 % based on the formation of Li4.4Si during alloying/dealloying processes, resulting in cracking and pulverization of the electrode and badly contacted with the currents, which makes it hardly to retain the long cyclic performance [2][3][4]; the other one is the unstable solid electrolyte interface (SEI) formation during the lithium ion insertion and deinsertion process [5][6][7]. Recently, different Si nano/micro-structures such as nanotubes [8][9], nanorods [10], nanowires [11][12][13], nanoparticles [14][15], thin films [16][17], and mesoporous structures [18][19][20] has been synthesized to improve the cyclic performance. Meanwhile, the protection of the anode from the directly contacting with the electrolyte to form stable SEI film has been approved to be another choice to enhance the cyclic performance. SiO 2 , the natural silicon oxide, has been chosen to act as the separation [21][22][23][24][25][26] between the anode and the electrolyte to stabilize SEI films. The SiO 2 layer is also easy to form and could accommodate the volume expansion during charge/discharge process. Cui's group synthesized a novel double-walled Si nanotube with a thin SiO 2 layer outside, leading to a stable SEI film [9]. The Si/ SiO 2 nanotube shows excellent cyclic performance over 6000 cycles. However, most SiO 2 -coated Si particles show very low capacity even at a low current due to the non-conductivity of the SiO 2 layer. For example, Su et al. [24] synthesized a double shell Si/SiO 2 /C nanocomposites, in which the SiO 2 was coated by decomposed with Li 2 SO4. They showed that both of the SiO 2 and the carbon layers could accommodate the volume expansion of Si, leading to good cycling stability. A reversible capacity of 800 mAhg -1 is achieved at a very low current of 50 mAg-1 after 30 cycles. However, the rate capacity is dissatisfactory due to the non-conductive of the SiO 2 . Therefore, it is a great challenge to further improve cycling performance by using the above-mentioned strategies.
Herein, we report a simple, convenient way to synthesize porous Si/SiO 2 /C particles. A comparable capacity of 550 mAhg -1 is achieved even at a high current of 800 mAg-1 after 30 cycles with a relatively thick SiO 2 layer. The double layers of the SiO 2 and carbon can not only buffer the volume expansion, but also form a stable SEI film.  Mg 2 Si (purity, >90%) was purchased from Zhejiang YHL New Energy Material Corporation. At first, 0.5 g Mg 2 Si was annealed at 700 °C in the air for 20 h in a tube furnace. After cooling down to room temperature, the product was treated by the hydrochloric acid (HCl) solution (0.2 molL-1) for 30 min. After washed with deionized water and ethanol for three times, the product was centrifuged and collected. Finally, the product was dried at 80 °C for 6 h in the air. For coating of a carbon layer, 0.2 g products was annealed at 600 °C for 2 h in a mix gas flowing (C 2 H 2 :Ar = 1:10, volume ratio) in a tube furnace.

Characterization
A Rigaku D/max-ga x-ray diffractometer with graphite monochromatized Cu Kα radiation (γ = 1.54178 Å) was used to detect the samples. The morphologies and the structures were characterized by the scanning electron microscopy (SEM, Hitachi S4800) and transmission electron microscopy (TEM, JEM-200 CX, 160 kV) and high-resolution transmission electron microscopy (HRTEM, JEOL JEM-2010).

Electrochemical performance
Electrochemical performance was carried out using the half-cell testing method with the lithium metal as the counter and reference anode. Briefly, Si/SiO 2 /C, acetylene black (AB), polyvinylidene fluoride (PVDF), with a mass ratio of 75: 15: 10, were mixed and dissolved in the N-methyl-2pyrrolidine (NMP) to get an uniform slurry. After pasting on the copper foils and dried at 120 °C for 12 h under vacuum, the cells were assembled in an argon-filled glove box. The electrolyte was 1 M LiPF6 dissolved in a mixture of ethylene carbonate (EC) and diethyl carbonate (DEC) with the volume ratio of EC:DEC = 1:1. An Arbin BT 2100 system was used for the electrochemical performance. All cells were cycled in the range of 0.01~1.5 V at different current densities.  (Fig. 2a) that the size of the particles is 5~10 μm. In the high-magnified SEM images (Figs. 2b and c), many pores in the particles can be observed with the size of 50~200 nm. Fig. 2d shows the EDX pattern of the products. It can be seen that the elements Cu, Si, O and C can be detected, which are originated from the Cu substrate and Si/ SiO 2 /C particles, respectively. In order to further identify the SiO 2 and carbon layer, TEM and HRTEM analysis were employed. From the low-magnified TEM image (Fig. 3a) , we can see that the particles are composed of small particles ranging from 50 to 200 nm which are connected with each other to form a porous structure. Figs. 3b and c show the highmagnified TEM images of the porous Si/SiO 2 /C particles. The strong contrast between the core and outer layer indicates that an amorphous layer exists on the surface of the Si particles. The thickness of the amorphous layer is about 5~20 nm. It is well known that Si could be easily oxidized even at room temperature. The generated SiO 2 layer will prevent the inner silicon from oxidation, so the thickness of the SiO 2 is usually very thin at room temperature. In this case, the high annealing temperature could offer large driving force which would lead to continuous oxidation. Fig. 3d shows the HRTEM image of a porous Si/SiO 2 /C particle. As can be seen, the amorphous layer is composed of a SiO 2 layer and carbon layer, respectively. To further characterize the element distribution of the porous Si/SiO 2 /C particles, the EDX mapping was employed (Fig.4). It can be seen that Si and O show uniform distribution in a Si/ SiO 2 /C particle, while C only exists on the surface of the particle. This indicates that the oxidation of the Si is uniform, while the carbon doesn't penetrate into internal of the porous particle. Motivated by the core-shell structures, the electrochemical performance of porous Si/SiO 2 /C particles is tested as anode materials of Li-ion batteries. Fig. 5a is the cyclic voltammograms of the porous Si/SiO 2 /C particles at a scanning rate of 0.1 mVs-1. A distinct broad peak at ~0.8 V in the first charge profile is ascribed to the formation of SEI films on the surface of the active particles [24]. Below 0.2 V, a sharp reduction peak represents the insertion of lithium ion into Si, which is the typical anode peak of Si. After the first cycle, two oxidation peaks around 0.3 and 0.5 V, and a new reduction peak near 0.2 V are observed. All the multiple peaks are the representative processes of alloying and dealloying for amorphous silicon. Fig. 5b shows the first and second charge/discharge curves of the porous Si/SiO 2 /C particles measured at 0.2 C in the voltage range of 0.01~1.5 V. It can be seen that the charge and discharge platforms are consistent with the peaks in the CV curves. The first discharge capacity of the porous Si/SiO 2 /C particles is 3356.5 mAhg -1 , while the first charge capacity is 2107 mAhg -1 , resulting in the initial Coulombic efficiency of 62.8 %. The relatively low initial Coulombic efficiency is mainly due to the large surface area and the existence of SiO 2 layer.  Fig. 6a shows the Coulombic efficiency and discharge/charge capacity versus cycling numbers. It can be seen that the Coulombic efficiency increases to higher than 95 % after 10 cycles and even nearly 100 % after 20 cycles. A reversible discharge capacity of 550 mAhg -1 is remained after 30 cycles at a current density of 0.2 C (800 mAg-1), which is better than previous results [23,24]. The enhanced performance may be attributed to the following two reasons: the co-existence of SiO 2 and C layer could prevent the silicon core from directly contacting with the electrolyte, which may decrease the regeneration of the SEI film [9]; the core-shell and porous structure can accommodate the volume changes during alloying/de-alloying process. Fig. 6b shows the cycling performance for the porous Si/SiO 2 /C particles at different current densities. As observed, the specific capacity fades fast along with the increasing current. When the current density recovers to 0.8 Ag-1, the capacity can restore to the previous state, indicating the good rate performance. Even at a very high current density, 3.2 Ag-1, a reversible capacity over 250 mAhg -1 is remained. The good rate capability of the porous Si/SiO 2 /C particles is due to the porous structure and the co-existence of SiO 2 and C layer to form a stable SEI film. It is believed that the cycling and rate performance can be further enhanced by adjusting the thickness of the SiO 2 and carbon layer, which is under investigation. Figure 6: (a) Capacity versus cycling numbers of the porous Si/SiO 2 /C particles at the testing current of 800 mAg-1; (b) Rate capability of the porous Si/SiO 2 /C particles.

Conclusion
In summary, the porous Si/SiO 2 /C particles were synthesized via the annealing of Mg 2 Si and subsequent carbon coating. When used as anode materials of Li-ion batteries, a reversible capacity over 550 mAhg -1 is retained at the current of 800 mAg-1 after 30 cycles. The cycling and rate performance is improved compared to bulk Si materials. The SiO 2 and carbon layer can not only protect the Si from directly contacting with the electrolyte, but also acts as the buffer to release